• Journal of Radiation Protection and Research
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• 제20권1호
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• pp.25-36
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• 1995

The purpose of this research is to develop stereotactic localization and radiation measurement system for the efficient and precise radiosurgery. The algorithm to obtain a 3-D stereotactic coordinates of the target has been developed using a Fisher CT or angio localization. The procedure of stereotactic localization was programmed with PC computer, and consists of three steps: (1) transferring patient images into PC; (2) marking the position of target and reference points of the localizer from the patient image; (3) computing the stereotactic 3-D coordinates of target associated with position information of localizer. Coordinate transformation was quickly done on a real time base. The difference of coordinates computed from between Angio and CT localization method was within 2 mm, which could be generally accepted for the reliability of the localization system developed. We measured dose distribution in small fields of NEC 6 MVX linear accelerator using various detector; ion chamber, film, diode. Specific quantities measured include output factor, percent depth dose (PDD), tissue maximum ratio (TMR), off-axis ratio (OAR). There was small variation of measured data according to the different kinds of detectors used. The overall trends of measured beam data were similar enough to rely on our measurement. The measurement was performed with the use of hand-made spherical water phantom and film for standard arc set-up. We obtained the dose distribution as we expected. In conclusion, PC-based 3-D stereotactic localization system was developed to determine the stereotactic coordinate of the target. A convenient technique for the small field measurement was demonstrated. Those methods will be much helpful for the stereotactic radiosurgery.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2008년도 International Meeting on Information Display
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• pp.1261-1262
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• 2008

Laser-based crystallization techniques are ideally-suited for forming high-quality crystalline Si films on active-matrix display backplanes, because the highly-localized energy deposition allows for transformation of the as-deposited a-Si without damaging high-temperature-intolerant glass and plastic substrates. However, certain significant and non-trivial attributes must be satisfied for a particular method and implementation to be considered manufacturing-worthy. The crystallization process step must yield a Si microstructure that permits fabrication of thin-film transistors with sufficient uniformity and performance for the intended application and, the realization and implementation of the method must meet specific requirements of viability, robustness and economy in order to be accepted in mass production environments. In recent years, Low Temperature Polycrystalline Silicon (LTPS) has demonstrated its advantages through successful implementation in the application spaces that include highly-integrated active-matrix liquid-crystal displays (AMLCDs), cost competitive AMLCDs, and most recently, active-matrix organic light-emitting diode displays (AMOLEDs). In the mobile display market segment, LTPS continues to gain market share, as consumers demand mobile devices with higher display performance, longer battery life and reduced form factor. LTPS-based mobile displays have clearly demonstrated significant advantages in this regard. While the benefits of LTPS for mobile phones are well recognized, other mobile electronic applications such as portable multimedia players, tablet computers, ultra-mobile personal computers and notebook computers also stand to benefit from the performance and potential cost advantages offered by LTPS. Recently, significant efforts have been made to enable robust and cost-effective LTPS backplane manufacturing for AMOLED displays. The majority of the technical focus has been placed on ensuring the formation of extremely uniform poly-Si films. Although current commercially available AMOLED displays are aimed primarily at mobile applications, it is expected that continued development of the technology will soon lead to larger display sizes. Since LTPS backplanes are essentially required for AMOLED displays, LTPS manufacturing technology must be ready to scale the high degree of uniformity beyond the small and medium displays sizes. It is imperative for the manufacturers of LTPS crystallization equipment to ensure that the widespread adoption of the technology is not hindered by limitations of performance, uniformity or display size. In our presentation, we plan to present the state of the art in light sources and beam delivery systems used in high-volume manufacturing laser crystallization equipment. We will show that excimer-laser-based crystallization technologies are currently meeting the stringent requirements of AMOLED display fabrication, and are well positioned to meet the future demands for manufacturing these displays as well.

• 한국의학물리학회지:의학물리
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• 제22권3호
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• pp.148-154
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• 2011

TRS-398 프로토콜에서 중심전극에 대한 최근의 연구 결과들을 적용하여 선질인자($k_{Q,Q_0}$)를 평가하였다. 대상 전리함은 PTW-31010과 IBA-CC13이었다. 광자선 및 전자선 선질의 함수로서 선질인자를 계산하였으며 현재 TRS-398 프로토콜의 값들과 비교하였다. PTW-31010 전리함과 같이 알루미늄 전극으로 구성된 전리함에 대하여 새로운 보정을 취하는 경우에 선질인자가 광자선에서 최대 0.4% 그리고 전자선에서 최대 0.9% 증가하는 것으로 나타났다. 또한 IBA-CC13과 같이 C-552 전극을 사용하는 전리함의 경우에 기존의 보정체계를 그대로 적용할 수 있음을 확인하였다.

• 한국콘텐츠학회논문지
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• 제11권9호
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• pp.437-442
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• 2011

본 연구의 목적은 진단방사선촬영의 X-선 빔 조사 조건하에서 광자극발광선량계를 사용하여 환자의 피부선량을 측정하는 것이다. 피부선량의 측정은 머리, 가슴, 골반에 대하여 실시하고 재현성의 시험은 가슴에서 시행하였다. 그 결과 머리는 이마에서 피부선량 1.30 mSv의 값을 얻었으며 가슴은 검상돌기, 유방, 폐첨에서 각각 0.92, 0.52, 0.70 mSv의 값을 얻었다. 또한 골반은 좌측골반과 우측골반에서 피부선량 각각 2.78, 3.08 mSv의 값을 얻었다. 재현성은 변동계수로서 0.033을 얻었다. 피부선량들은 결정적 영향에서 일반인의 선량한도(50 mSv)의 1/100에서 1/17에 대응하는 값들을 나타냈다. 각 관전압에 대한 피부선량의 정확한 측정을 위하여 측정값은 판독장치의 표시값에 보정인자를 곱해야 한다. 이에 향후에는 관전압에 대한 에너지의존성의 연구가 진행되어야 할 것으로 사료된다.

• 한국방사선학회논문지
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• 제8권7호
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• pp.449-454
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• 2014

이 연구의 목적은 6 MV 광자 빔에 대하여 팬텀 표면으로부터 1 cm 깊이에서 조사야 가장자리 바깥 축외선량비와 1 mmPb의 차폐비를 조사하는 데 있다. 180 cGy의 선량은 SAD기법에서 $10{\times}10cm^2$와 $15{\times}15cm^2$ 조사야에 대하여 깊이 10 cm에 전달되었다. 축외선량비는 조사야의 중심축과 가장자리로부터 2, 4, 6 cm에 위치된 광자극형광나노닷선량계(OSLnD)들의 선량을 측정하여 계산하였다. 그리고 1 mmPb의 차폐비는 조사야 가장자리로부터 2, 4, 6 cm에 위치된 OSLnD들의 선량을 측정하여 산출하였다. 결과로서, $10{\times}10cm^2$와 $15{\times}15cm^2$ 조사야에 대하여, 축외선량비들은 0.008-0.023과 0.011-0.028을 각각 얻었다. 또한 1 mmPb의 차폐비들은 0.868-0.888과 0.807-0.842을 각각 얻었다. 이 결과들은 방사선치료 조사야 바깥에 위치한 위험장기들을 보호하기 위한 자료를 제공한다.

• 대한기관식도과학회지
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• 제15권2호
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• pp.49-56
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• 2009

Purpose : To evaluate the treatment outcome for patients with locally advanced, unresectable esophageal cancer treated with relatively high dose radiation therapy(RT). Materials and Methods : From January 2000 to December 2008, 32 patients with locally advanced unresectable or medically inoperable esophageal cancer were treated with radiation therapy(RT) with or without concurrent chemotherapy. Ten patients were excluded from analysis because of distant metastasis and drop off. Patient distributions according to AJCC stages II, III IVa were 7(31.8%), 12(54.6%), 3(13.6%) respectively. The locations of tumor were cervical/upper thorax 3 (13.6%), mid thorax 13(59.1%), and lower thorax/abdominal 6(27.3%), respectively. Eleven patients received RT only, and 11 patients received cisplatin based concurrent chemoradiotherapy(CCRT). Median radiation dose was 65 Gy(range 57.6~72 Gy). Results : The median follow-up was 9.1 months(range 1.9~43.8 months). The response rates for complete response, Partial response, stable disease and Persistent disease were 6(27.3%), 11(50.0%), 4(18.2%) and 1(4.5%), respectively. Two patients(9.1%) suffered from esophageal stenosis and stents were inserted. Two patients(9.1%) had Grade 3 radiation pneumonitis and one of them expired due to acute respiratory distress syndrome(ARDS) at 36 days after completion of radiation therapy. The recurrence rate was 11(50.0%). The patterns of recurrence were persistent disease and local progression in 5(22.7%), local recurrence 3(13.7%) and concomitant local and distant recurrence in 3(13.7%). The overall survival(OS) rate was 32.1% at 2 years and 21.4% at 3 years(median 12.0 months). Disease free survival(DFS) rate was 17.3% at 2 and 3 years. All patients who had no dysphagia at diagnosis showed complete response after treatment and 100% OS at 3 years(p=0.0041). The OS for above 64.8 Gy group and 64.8 Gy or below group at 3 years were 60.6% and 9.1%(p=0.1341). The response to treatment was the only significant factor affecting OS(p=0.004). Conclusion : Relatively high dose radiation therapy in unresectable esophageal cancer tended to have a better outcome without increased complication rate. Further study with more patients is warranted to justify improved result.

• Journal of Radiation Protection and Research
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• 제45권3호
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• pp.130-141
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• 2020

Background: Concrete activation in cyclotron vaults is a major concern associated with their decommissioning because a considerable amount of activated concrete is generated by secondary neutrons during the operation of cyclotrons. Reducing the amount of activated concrete is important because of the high cost associated with radioactive waste management. This study aims to investigate the capability of the neutron absorbing materials to reduce concrete activation. Materials and Methods: The Particle and Heavy Ion Transport code System (PHITS) code was used to simulate a cyclotron target and room. The dimensions of the room were 457 cm (length), 470 cm (width), and 320 cm (height). Gd₂O₃, B₄C, polyethylene (PE), and borated (5 wt% ^natB) PE with thicknesses of 5, 10, and 15 cm and their different combinations were selected as neutron absorbing materials. They were placed on the concrete walls to determine their effects on thermal neutrons. Thin B₄C and Gd₂O₃ were placed between the concrete wall and additional PE shield separately to decrease the required thickness of the additional shield, and the thermal neutron flux at certain depths inside the concrete was calculated for each condition. Subsequently, the optimum combination was determined with respect to radioactive waste reduction, price, and availability, and the total reduced radioactive concrete waste was estimated. Results and Discussion: In the specific conditions considered in this study, the front wall with respect to the proton beam contained radioactive waste with a depth of up to 64 cm without any additional shield. A single layer of additional shield was inefficient because a thick shield was required. Two-layer combinations comprising 0.1- or 0.4-cm-thick B₄C or Gd₂O₃ behind 10 cm-thick PE were studied to verify whether the appropriate thickness of the additional shield could be maintained. The number of transmitted thermal neutrons reduced to 30% in case of 0.1 cm-thick Gd₂O₃+10 cm-thick PE or 0.1 cm-thick B₄C+10 cm-thick PE. Thus, the thickness of the radioactive waste in the front wall was reduced from 64 to 48 cm. Conclusion: Based on price and availability, the combination of the 10 cm-thick PE+0.1 cmthick B₄C was reasonable and could effectively reduce the number of thermal neutrons. The amount of radioactive concrete waste was reduced by factor of two when considering whole concrete walls of the PET cyclotron vault.

• Asian Pacific Journal of Cancer Prevention
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• 제17권7호
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• pp.3643-3646
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• 2016

Management of eyelid cancers is based on surgery and/or radiotherapy (RT). The treatment objective is to control tumors with acceptable functional and esthetic outcomes. The aim of this study was to evaluate the results of radiation therapy in management of epithelial eyelid cancers, reviewing retrospectively the clinical records of patients treated in our institution from January 1989 to December 2013. We focused on clinical and histological features, treatment characteristics, tolerance and disease control. One hundred and eight patients (62 men and 46 women) were enrolled, with a mean age of 61 years [ranges 15-87]. The most frequent tumor location was the inner canthus (42.6%). Median tumor size was 21 mm [ranges 4-70]. Histological type was basal cell carcinoma in 88 cases (81.5%), squamous cell carcinoma in 16 (14.8%) and sebaceous carcinoma in 4 (3.7%). Radiation therapy was exclusive in 67 cases (62%) and post-operative for positive or close margins in the remaining cases. Kilovoltage external beam radiotherapy (KVRT) was used in 63 patients (58.3%) and low-dose-rate interstitial brachytherapy in 37 (34.3%). Eight (7.4%) were treated with cobalt or with a combination of KVRT-cobalt, KVRT-electron beams, KVRT-brachytherapy or cobalt-electron beams. The total delivered radiation doses were 70 Gy (2 Gy/fraction) in 62 patients (57.4%), 66 Gy (2 Gy/fraction) in 37 (34.3%) and 61.2 Gy (3.4Gy/fraction) in 9 (8.3%). After a median follow-up of 64 months, we noted 10 cases of local recurrences(9.2%): 7 after exclusive and 3 after post-operative RT. No local recurrence occurred in patients treated with brachytherapy. Actuarial 5-year local recurrence-free rate, disease-free survival and overall survival were respectively 90%, 90% and 97%. T-stage was found to be a significant factor for recurrence (p=0.047). All acute radiation-related reactions were scored grade I or II. Delayed effects were eye watering in 24 cases (22.2%), eye dryness in 19 (17.6%), unilateral cataract in 7 (6.4%) and ectropion in 4 (3.7%). Radiation therapy and especially brachytherapy is an efficient treatment of eyelid cancers, allowing eye conservation and functional preservation with good local control rates and acceptable toxicity.

• 한국의학물리학회지:의학물리
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• 제18권4호
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• pp.221-225
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• 2007

움직이는 자기장을 이용한 팬텀 속 선량 변조에 관한 몬테칼로 계산을 수행하였다. 본 연구의 목적은 빔 축을 따라 이동하는 횡 자기장을 이용하여 특정감이 영역에 균일한 선량을 얻는 것이다. 이를 위해 두 가지 구성 즉, 깊이 방향으로 일정한 속도 그리고 점차 감소하는 속도를 가지는 자기장에 대해 깊이 선량율을 구하였다. 연속적 움직임에 대한 근사로서 단계별 이동과 시간인자를 도입하였다. 위치별 정지한 자기장 대한 김이 선량율 자료에 최소제곱법을 적용하여 자기장 위치에 따른 최적의 시간인자를 구하였다. 몬테칼로 계산결과를 통하여 자기장의 속도를 변화시킴으로써 평탄한 선량 분포를 얻을 수 있음을 확인하였다. 이 때 3 T 자기장 세기에 대한 계산결과 평탄 영역의 선량은 자기장이 없을 때에 비해 약 10.1% 증가하는 것으로 나타났다.

• Radiation Oncology Journal
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• 제11권1호
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• pp.43-50
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• 1993

방사선에의 노출은 염색체 이상을 유발하는 원인으로 널리 인식되고 있으나 in vivo상태에서 방사선 조사 후 발생되는 염색체 이상의 종류와 빈도 규명은 드물었다. 이에 본 연구에서는 암 환자에서 방사선 치료 전 및 후에 말초혈액 임파구의 염색체 변이를 비교 관찰하고 방사선 조사에 의해 암 환자세포에서 나타나는 염색체 이상에서 절단점의 분포가 암 발생과 밀접한 연관이 된 유전자 및 염색체의 재조합이 자주 일어나는 부위와 연관관계 가 있음을 규명하고자 하였다. 25예의 암 환자에서 방사선 치료가 시작되기 전과 $4000\~7000cGy$의 근치적 방사선치료가 끝난 직후 말초 혈액을 채취하여 임파구를 배양후 G-분염법을 이용하여 염색한 후 환자마다 방사선치료 전후로 각각 30개씩의 증기상을 관찰하였다. 치료전에 염색체 이상을 나타낸 세포 분열 중기상의 빈도는 $4.93\%$로 정상 대조군 집단의 빈도 $2\%$보다 높았다(p<0.05). 방사선 치료후 염색체 이상 세포의 빈도는 $22.13\%$로 치료전에 비해 매우 중가되었다(p<0.01). 또한 세포 중기상당 이상 염색체의 수도 치료전과 후가 각각 1.49및 2.14로 치료후 증가 되었다(p<0.05). 염색체 이상의 종류는 major chromosomal aberration 특히 구조적 이상의 빈도가 치료전보다 후에 $65.45\%$에서 $88.45\%$로 증가되었고 minor structural abnormality와 수적 변이의 빈도는 감소되었다. 방사선 치료후 염색체 절단점의 수가 2개 이상인 경우가 단일 절단점을 가진 이상에 비해 증가되었다. 절단점의 분포에 있어서는 암세포에서 가장 흔한 이상을 나타내는 1번 및 3번 염색체와 절단점의 증가가 암 발생관 연관된다고 보고된 8번 및 11번 염색체에서 본 연구결과 기대치 이상의 절단점의 분포를 보이고, 암 세포에서 드물게 이상을 나타내는 13, 15및 21번 염색체에서는 기대치 보다 감소된 절단점의 분포를 보였다. 따라서 방사선 치료 후 염색체 이상의 빈도는 증가되었으며 방사선 조사에 의해 나타나는 염색체의 절단점의 분포는 암 발생과 밀접한 연관이 된 유전자 및 염색체의 재조합이 자주 일어나는 부위와 밀접한 연관 관계가 있음을 보여 주었다.